Titlebook: Continuum Mechanics and Theory of Materials; Peter Haupt Textbook 2002Latest edition Springer-Verlag Berlin Heidelberg 2002 Continuum Mech

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Der Essay: Erkenntnis und Existenz,have in an entirely different way, given the same external conditions. Accordingly, constitutive equations have to be distinguished from general laws of nature referring to kinematics and balance relations. They are ., intended to reflect the characteristic features of the actual material behaviour

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,Sind wir reif für die »Moralpille«?,umption of objectivity to use the material time derivatives to establish evolution equations for internal variables, which are either of . strain or . stress type. In view of the material description’s independence of the reference system, there should not be any objections, therefore, to using excl

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Classical Theories of Continuum Mechanics,have in an entirely different way, given the same external conditions. Accordingly, constitutive equations have to be distinguished from general laws of nature referring to kinematics and balance relations. They are ., intended to reflect the characteristic features of the actual material behaviour

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Constitutive Models in Thermomechanics, the principle of irreversibility (second law). The formulation of the principle of irreversibility usually employed in continuum thermomechanics has its roots in the entropy production (3.39), . and demands that this must be non-negative:

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1439-2674 ory of viscoelasticity. This leads to a new theory of finite linear viscoelasticity of incompressible isotropic materials. Anisotropic viscoplasticity is completely reformulated and extended to a general constitutive theory that covers crystal plasticity as a special case.978-3-642-07718-0978-3-662-04775-0Series ISSN 1439-2674

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Balance Relations of Mechanics,with the influence of the outside world. This interaction is described by the balance relations. The basic idea is the free-body principle, described in the following physical definition, which is complementary to Definition 1. 1 from a physical point of view.